Wavelength division multiplexing/demultiplexing devices using diffractive optic lenses

ABSTRACT

An improved wavelength division multiplexing device is disclosed. The improved wavelength division multiplexing device has a diffraction grating for combining a plurality of monochromatic optical beams into a multiplexed, polychromatic optical beam. The improvement in the improved wavelength division multiplexing device is the use of a diffractive optic collimating/focusing lens for collimating the plurality of monochromatic optical beams traveling along a first direction to the diffraction grating, and for focusing the multiplexed, polychromatic optical beam traveling along a second direction from the diffraction grating, wherein the second direction being substantially opposite the first direction.

CROSS-REFERENCE TO RELATED APPLICATIONS

This patent application is a continuation-in-part patent application of U.S. patent application Ser. No. 08/990,197, filed Dec. 13, 1997 (now U.S. Pat. No. 6,011,884), and U.S. patent application Ser. No. 08/990,199, filed Dec. 13, 1997 (now U.S. Pat. No. 5,999,672), both of which are hereby incorporated by reference herein in their entirety.

This patent application is related to U.S. patent application Ser. No. 09/363,042, filed concurrently herewith and hereby incorporated by reference herein in its entirety.

FIELD OF THE INVENTION

The present invention relates generally to wavelength division multiplexing/demultiplexing and, more particularly, to wavelength division multiplexing/demultiplexing devices using diffractive optic lenses.

BACKGROUND OF THE INVENTION

Wavelength division multiplexing (WDM) is a rapidly emerging technology that enables a very significant increase in the aggregate volume of data that can be transmitted over optical fibers. Prior to the use of WDM, most optical fibers were used to unidirectionally carry only a single data channel at one wavelength. The basic concept of WDM is to launch and retrieve multiple data channels in and out, respectively, of an optical fiber. Each data channel is transmitted at a unique wavelength, and the wavelengths are appropriately selected such that the channels do not interfere with each other, and the optical transmission losses of the fiber are low. Today, commercial WDM systems exist that allow for the transmission of 2 to 100 simultaneous data channels.

WDM is a cost-effective method of increasing the volume of data (commonly termed bandwidth) transferred over optical fibers. Alternate competing technologies for increasing bandwidth include the burying of additional fiber optic cable or increasing the optical transmission rate over optical fiber. The burying of additional fiber optic cable is quite costly as it is presently on the order of $15,000 to $40,000 per kilometer. Increasing the optical transmission rate is limited by the speed and economy of the electronics surrounding the fiber optic system. One of the primary strategies for electronically increasing bandwidth has been to use time division multiplexing (TDM), which groups or multiplexes multiple lower rate electronic data channels together into a single very high rate channel. This technology has for the past 20 years been very effective for increasing bandwidth. However, it is now increasingly difficult to improve transmission speeds, both from a technological and an economical standpoint. WDM offers the potential of both an economical and technological solution to increasing bandwidth by using many parallel channels. Further, WDM is complimentary to TDM. That is, WDM can allow many simultaneous high transmission rate TDM channels to be passed over a single optical fiber.

The use of WDM to increase bandwidth requires two basic devices that are conceptually symmetrical. The first device is a wavelength division multiplexer. This device takes multiple beams, each with discrete wavelengths that are initially spatially separated in space, and provides a means for spatially combining all of the different wavelength beams into a single polychromatic beam suitable for launching into an optical fiber. The multiplexer may be a completely passive optical device or may include electronics that control or monitor the performance of the multiplexer. The input to the multiplexer is typically accomplished with optical fibers, although laser diodes or other optical sources may also be employed. As mentioned above, the output from the multiplexer is a single polychromatic beam which is typically directed into an optical fiber.

The second device for WDM is a wavelength division demultiplexer. This device is functionally the opposite of the wavelength division multiplexer. That is, the wavelength division demultiplexer receives a polychromatic beam from an optical fiber and provides a means of spatially separating the different wavelengths of the polychromatic beam. The output from the demultiplexer is a plurality of monochromatic beams which are typically directed into a corresponding plurality of optical fibers or photodetectors.

During the past 20 years, various types of WDMs have been proposed and demonstrated. For example, (1) W. J. Tomlinson, Applied Optics, Vol. 16, No. 8, pp. 2180-2194 (August 1977); (2) A. C. Livanos et al., Applied Physics Letters, Vol. 30, No. 10, pp. 519-521 (May 15, 1977); (3) H. Ishio et al., Journal of Lightwave Technology, Vol 2, No. 4, pp. 448-463 (August 1984); (4) H. Obara et al., Electronics Letters, Vol. 28, No. 13, pp. 1268-1270 (Jun. 18, 1992); (5) A. E. Willner et al., IEEE Photonics Technology Letters, Vol. 5, No. 7, pp. 838-841 (July 1993); and (6) Y. T. Huang et is al., Optical Letters, Vol. 17, No. 22, pp. 1629-1631 (Nov. 15, 1992), all disclose some form of WDM device and/or method. However, the WDM devices and/or methods disclosed in the above-listed publications are all classical optics-based WDM approaches which employ very basic lenses that are adequate only for use with multimode optical fibers and are inadequate for use with single mode optical fibers because the core diameter of a single mode optical fiber (i.e., typically 8 μm) is much smaller than the core diameter of a multimode optical fiber (i.e., typically 62.5 μm). That is, due to the very basic lenses employed therein, WDM devices incorporating the principles set forth in the classical optics-based WDM approaches disclosed in the above-listed publications are unable to receive and transmit optical beams from and to single mode optical fibers, respectively, without incurring unacceptable amounts of insertion loss and channel crosstalk. These unacceptable levels of insertion loss and channel crosstalk are largely due to the inadequate imaging capabilities of these very basic lenses, which are typically formed of standard optical glass materials.

One proposed solution to the above-described optical imaging problem has been to add additional lenses formed of standard optical glass materials to WDM devices, thereby resulting in WDM devices having doublet, triplet, and even higher number lens configurations. By adding these additional lenses to WDM devices, wherein the added lenses typically have alternating high and low refraction indexes, aberrations caused mainly by the spherical nature of the lenses are effectively canceled out. However, an increased cost is associated with adding these additional lenses due to the direct cost of the additional lenses, as well as the indirect costs associated with the increased complexity and resulting decreased manufacturability of WDM devices having multiple lenses.

Another proposed solution to the above-described optical imaging problem has been to use gradient refractive index lenses (e.g., Gradium lenses) in WDM devices. The use of these gradient refractive index lenses results in a significant improvement in the quality of the imaging system within WDM devices. However, costs associated with manufacturing these gradient refractive index lenses is significantly greater than the costs associated with manufacturing standard homogeneous index lenses, despite the fact that both are typically formed of standard optical glass materials.

In view of the foregoing, there remains a real need for a WDM device which possesses or allows for all the characteristics of: low cost, component integration, environmental and thermal stability, low channel crosstalk, low channel signal loss, ease of interfacing, large number of channels, and narrow channel spacing. Accordingly, it would be desirable to provide a WDM device which overcomes the above-described inadequacies and shortcomings, while possessing or allowing for all of the above-stated characteristics.

OBJECTS OF THE INVENTION

The primary object of the present invention is to provide wavelength division multiplexing/demultiplexing devices which use diffractive optic lenses to achieve increased device performance, as well as reduced device cost, complexity, and manufacturing risk.

The above-stated primary object, as well as other objects, features, and advantages, of the present invention will become readily apparent from the following detailed description which is to be read in conjunction with the appended drawings.

SUMMARY OF THE INVENTION

According to the present invention, an improved wavelength division multiplexing device is provided. In a preferred embodiment, the improved wavelength division multiplexing device has a diffraction grating for combining a plurality of monochromatic optical beams into a multiplexed, polychromatic optical beam. The improvement in the improved wavelength division multiplexing device comes from the use of a diffractive optic collimating/focusing lens for collimating the plurality of monochromatic optical beams traveling along a first direction to the diffraction grating, and for focusing the multiplexed, polychromatic optical beam traveling along a second direction from the diffraction grating. The second direction is substantially opposite the first direction. The diffraction grating is typically a reflective diffraction grating oriented at the Littrow diffraction angle with respect to the first and second directions.

The diffractive optic collimating/focusing lens has substantially planar front and back surfaces, and a microscopic pattern associated with the diffractive optic can be formed on either the substantially planar front surface or the substantially planar back surface. The diffractive optic collimating/focusing lens can be one of several types such as, for example, a binary diffractive optic lens or a Fresnel diffractive optic lens.

The diffractive optic collimating/focusing lens typically operates in the infrared (IR) region of the electromagnetic spectrum since this is the region where the power loss (attenuation) and dispersion of silica-based optical fibers is very low. Accordingly, the diffractive optic collimating/focusing lens is typically formed of a material selected from the group consisting of glass, crystalline, and plastic, as well as from any of a number of other appropriate materials that efficiently transmit optical beams in the infrared (IR) region of the electromagnetic spectrum.

In accordance with other aspects of the present invention the improvement in the improved wavelength division multiplexing device can be the use of a diffractive optic collimating lens for collimating the plurality of monochromatic optical beams traveling along a first direction to the diffraction grating, and a diffractive optic focusing lens for focusing the multiplexed, polychromatic optical beam traveling along a second direction from the diffraction grating. In this case, the second direction is different from, but not opposite, the first direction.

In accordance with other aspects of the present invention, an integrated wavelength division multiplexing device can be provided. That is, an integrated wavelength is division multiplexing device can be provided comprising a diffractive optic collimating/focusing lens for collimating a plurality of monochromatic optical beams traveling along a first direction, and for focusing a multiplexed, polychromatic optical beam traveling along a second direction. In this case, the second direction is again substantially opposite the first direction.

The integrated wavelength division multiplexing device also comprises a first homogeneous index boot lens affixed to the diffractive optic collimating/focusing lens for transmitting the plurality of monochromatic optical beams from the diffractive optic collimating/focusing lens along the first direction, and for transmitting the multiplexed, polychromatic optical beam to the diffractive optic collimating/focusing lens along the second direction. The first homogeneous index boot lens has a planar interface surface.

The integrated wavelength division multiplexing device further comprises a diffraction grating formed at the planar interface surface of the first homogeneous index boot lens for combining the plurality of monochromatic optical beams into the multiplexed, polychromatic optical beam, and for reflecting the multiplexed, polychromatic optical beam back into the first homogeneous index boot lens. The diffraction grating is typically a reflective diffraction grating oriented at the Littrow diffraction angle with respect to the first and second directions.

In accordance with further aspects of the present invention, the homogeneous index boot lens can be incorporated into the diffractive optic collimating/focusing lens such that the diffractive optic collimating/focusing lens has the planar interface surface at which the diffraction grating is formed.

In accordance with still further aspects of the present invention, the diffractive optic collimating/focusing lens can have a planar interface surface for accepting the plurality of monochromatic optical beams from at least one optical source (e.g., optical fibers, laser diodes), and for outputting the multiplexed, polychromatic optical beam to at least one optical receiver (e.g., optical fibers, photodetectors).

In accordance with still further aspects of the present invention, the integrated wavelength division multiplexing device further comprises a second homogeneous index boot lens affixed to the diffractive optic collimating/focusing lens for transmitting the plurality of monochromatic optical beams to the diffractive optic collimating/focusing lens along the first direction, and for transmitting the multiplexed, polychromatic optical beam from the diffractive optic collimating/focusing lens along the second direction. The second homogeneous index boot lens preferably has a planar interface surface for accepting the plurality of monochromatic optical beams from at least one optical source, and for outputting the multiplexed, polychromatic optical beam to at least one optical receiver.

In accordance with other aspects of the present invention, a wavelength division multiplexing device can be provided. That is, a wavelength division multiplexing device can be provided comprising a diffractive optic collimating lens for collimating a plurality of monochromatic optical beams, and a diffraction grating for combining the plurality of collimated, monochromatic optical beams into a multiplexed, polychromatic optical beam, and for reflecting the multiplexed, polychromatic optical beam. The wavelength division multiplexing device also comprises a diffractive optic focusing lens for focusing the reflected, multiplexed, polychromatic optical beam.

In accordance with further aspects of the present invention, the wavelength division multiplexing device can further comprise at least one reflecting element for reflecting the plurality of collimated, monochromatic optical beams toward the diffraction grating, and/or at least one reflecting element for reflecting the reflected, multiplexed, polychromatic optical beam toward the diffractive optic focusing lens.

At this point it should be noted that the above-described improved wavelength division multiplexing device, integrated wavelength division multiplexing device, and wavelength division multiplexing device are all bidirectional devices. Thus, the improved wavelength division multiplexing device can also be an improved wavelength division demultiplexing device, the integrated wavelength division multiplexing device can also be an integrated wavelength division demultiplexing device, and the wavelength division multiplexing device can also be a wavelength division demultiplexing device.

BRIEF DESCRIPTION OF THE DRAWINGS

In order to facilitate a fuller understanding of the present invention, reference is now made to the appended drawings. These drawings should not be construed as limiting the present invention, but are intended to be exemplary only.

FIG. 1a is a side view of a wavelength division multiplexing device having a diffractive optic collimating/focusing lens and a reflective diffraction grating in accordance with the present invention.

FIG. 1b is a top view of the wavelength division multiplexing device shown in FIG. 1a.

FIG. 1c is a perspective end view of a portion of the wavelength division multiplexing device shown in FIG. 1a.

FIG. 2a is an end and a cross-sectional view of a binary diffractive optic lens having a concentric circular pattern of steps surrounding a center raised region etched into the lens material.

FIG. 2b is an end and a cross-sectional view of a Fresnel diffractive optic lens having a concentric circular pattern of peaks surrounding a center raised region applied to the lens material.

FIG. 3a is a perspective view of a coupling device containing a plurality of laser diodes for replacing the plurality of optical input fibers in the multiplexing device shown in FIG. 1a.

FIG. 3b is a perspective view of a coupling device containing a plurality of photodetectors for replacing the plurality of optical input fibers in the demultiplexing device shown in FIG. 4a.

FIG. 4a is a side view of a wavelength division demultiplexing device having a diffractive optic collimating/focusing lens and a reflective diffraction grating in accordance with the present invention.

FIG. 4b is a top view of the wavelength division multiplexing device shown in FIG. 4a.

FIG. 5a is a side view of an integrated wavelength division multiplexing device having a diffractive optic collimating/focusing lens and a reflective diffraction grating in accordance with the present invention.

FIG. 5b is a top view of the integrated wavelength division multiplexing device shown in FIG. 5a.

FIG. 6a is a side view of an integrated wavelength division multiplexing device having a front extended diffractive optic collimating/focusing lens and a reflective diffraction grating in accordance with the present invention.

FIG. 6b is a top view of the integrated wavelength division multiplexing device shown in FIG. 6a.

FIG. 7a is a side view of an integrated wavelength division multiplexing device having a back extended diffractive optic collimating/focusing lens and a reflective diffraction grating in accordance with the present invention.

FIG. 7b is a top view of the integrated wavelength division multiplexing device shown in FIG. 7a.

FIG. 8 is a side view of a wavelength division multiplexing device using a diffractive optic collimating lens, a diffractive optic focusing lens, and a reflective diffraction grating in accordance with the present invention.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

Referring to FIGS. 1a and 1 b, there are shown a side view and a top view, respectively, of a preferred embodiment of a wavelength division multiplexing device 10 in accordance with the present invention. The multiplexing device 10 comprises a plurality of optical input fibers 12, an input fiber coupling device 14, a diffractive optic collimating/focusing lens 16, a reflective diffraction grating 18, an output fiber coupling device 20, and a single optical output fiber 22. All of the above-identified components of the multiplexing device 10 are disposed along an optical axis X—X of the multiplexing device 10, as will be described in more detail below.

At this point it should be noted that the optical input fibers 12 and the optical output fiber 22, as well as any other optical fibers described herein as being used in conjunction with WDM devices in accordance with the present invention, are single mode optical fibers. Of course, however, this does not limit the present invention WDM devices to use with only single mode optical fibers. For example, the present invention WDM devices can also be used with multimode optical fibers.

It should also be noted that the multiplexing device 10, as well as any other WDM devices described herein as being WDM devices in accordance with the present invention, is operating in the infrared (IR) region of the electromagnetic spectrum as a dense wavelength division multiplexing (DWDM) device (i.e., operating with data channels having channel spacings of 1 nm or less). Of course, however, this does not limit the present invention WDM devices to being only DWDM devices. For example, the present invention WDM devices can also be standard WDM devices (i.e., operating with data channels having channel spacings greater than 1 nm).

Returning to FIGS. 1a and b, the plurality of optical input fibers 12 are grouped into a one-dimensional input fiber array (i.e., a 1×4 array) by the input fiber coupling device 14, while the single optical output fiber 22 is secured to the output fiber coupling device 20. Both the input fiber coupling device 14 and the output fiber coupling device 20 are used for purposes of ease of optical fiber handling and precision placement, and can be formed of, for example, a silicon V-groove assembly. Referring to FIG. 1c, there is shown a perspective end view of a portion of the multiplexing device 10 revealing how the plurality of optical input fibers 12 are grouped into the one-dimensional input fiber array by the input fiber coupling device 14, and how the single optical output fiber 22 is secured to the output fiber coupling device 20. FIG. 1c also shows a monochromatic optical input beam 24 being transmitted from each of the plurality of optical input fibers 12, and a single multiplexed, polychromatic optical output beam 26 being transmitted to the single optical output fiber 22.

Each of the monochromatic optical input beams 24 being transmitted from the plurality of optical input fibers 12 is carrying a single channel of data at a unique wavelength, which is preferably, but not required to be, within the infrared (IR) region of the electromagnetic spectrum. The single channel of data that is being carried by each monochromatic optical input beam 24 is superimposed on each corresponding unique wavelength by means (e.g., laser diodes connected to the plurality of optical input fibers 12), which are not shown here and which do not form a part of this invention, but are well known in the art. The unique wavelengths of the monochromatic optical input beams 24 are appropriately preselected such that the data channels do not interfere with each other (i.e., there is sufficient channel spacing), and the optical transmission losses through both the optical input fibers 12 and the optical output fiber 22 are low, as is also well known in the art.

The single multiplexed, polychromatic optical output beam 26 being transmitted to the single optical output fiber 22 is carrying a plurality of channels of data at the unique wavelengths of each of the plurality of monochromatic optical input beams 24. The plurality of monochromatic optical input beams 24 are combined into the single multiplexed, polychromatic optical output beam 26 through the combined operation of the diffractive optic collimating/focusing lens 16 and the reflective diffraction grating 18, as will be described in more detail below.

At this point it should be noted that the input fiber coupling device 14 and the output fiber coupling device 20 are disposed offset from, but symmetrically about, the optical axis X—X of the multiplexing device 10 so as to insure that the single multiplexed, polychromatic optical output beam 26 is directed to the single optical output fiber 22 secured to the output fiber coupling device 20, and not to any of the plurality of optical input fibers 12 secured to the input fiber coupling device 14, or anywhere else. This offset spacing of the input fiber coupling device 14 and the output fiber coupling device 20 is determined based upon the focusing power of the diffractive optic collimating/focusing lens 16, as well as the characteristics of the diffraction grating 18 and the wavelengths of each of the monochromatic optical input beams 24.

Referring again to FIGS. 1a and 1 b, each of the plurality of monochromatic optical input beams 24 are transmitted from their corresponding optical input fiber 12 into the air space between the input fiber coupling device 14 and the diffractive optic collimating/focusing lens 16. Within this air space, the plurality of monochromatic optical input beams 24 are expanded in diameter until they become incident upon the diffractive optic collimating/focusing lens 16. The diffractive optic collimating/focusing lens 16 collimates each of the plurality of monochromatic optical input beams 24, and then transmits each collimated, monochromatic optical input beam 24′ to the reflective diffraction grating 18.

At this point it should be noted that the optical axis of the diffractive optic collimating/focusing lens 16 coincides with the optical axis X—X of the multiplexing device 10 so as to insure that the single multiplexed, polychromatic optical output beam 26 is directed to the single optical output fiber 22 secured to the output fiber coupling device 20, and not to any of the plurality of optical input fibers 12 secured to the input fiber coupling device 14, or anywhere else, as will be described in more detail below.

The reflective diffraction grating 18 operates to angularly disperse the plurality of collimated, monochromatic optical input beams 24′ by an amount that is dependent upon the wavelength of each of the plurality of collimated, monochromatic optical input beams 24′. Further, the reflective diffraction grating 18 is oriented at a special angle (i.e., the Littrow diffraction angle, a,) relative to the optical axis X—X of the multiplexing device 10 in order to obtain the Littrow diffraction condition for an optical beam having a wavelength that lies within or near the wavelength range of the plurality of collimated, monochromatic optical input beams 24′. The Littrow diffraction condition requires that an optical beam be incident on and reflected back from a reflective diffraction grating at the exact same angle. Therefore, it will be readily apparent to one skilled in the art that the reflective diffraction grating 18 is used to obtain near-Littrow diffraction for each of the plurality of collimated, monochromatic optical input beams 24′.

The Littrow diffraction angle, α_(i), is determined by the well-known diffraction grating equation,

mλ=2d(sin α_(i))

wherein m is the diffraction order, λ is the wavelength, d is the diffraction grating groove spacing, and α_(i) is the common angle of incidence and reflection. It will be readily apparent to one skilled in the art that the Littrow diffraction angle, α_(i), depends upon numerous variables, which may be varied as necessary to optimize the performance of the multiplexing device 10. For example, variables affecting the Littrow diffraction angle, α_(i), include the desired grating diffraction order, the grating blaze angle, the number of data channels, the spacing of the data channels, and the wavelength range of the multiplexing device 10.

At this point it should be noted that the reflective diffraction grating 18 can be formed from a variety of materials and by a variety of techniques. For example, the reflective diffraction grating 18 can be formed by a three-dimensional hologram in a polymer medium, or by replicating a mechanically ruled master with a polymer material. In both cases, the polymer is overcoated with a thin, highly reflective metal layer such as, for example, gold or aluminum. Alternatively, the reflective diffraction grating 18 can be formed by chemically etching into a planar material such as, for example, glass or silicon, which is also overcoated with a thin, highly reflective metal layer such as, for example, gold or aluminum.

As previously mentioned, the reflective diffraction grating 18 operates to angularly disperse the plurality of collimated, monochromatic optical input beams 24′. Thus, the reflective diffraction grating 18 removes the angular separation of the plurality of collimated, monochromatic optical input beams 24′, and reflects a single collimated, polychromatic optical output beam 26′ back towards the diffractive optic collimating/focusing lens 16. The single collimated, polychromatic optical output beam 26′ contains each of the unique wavelengths of the plurality of collimated, monochromatic optical input beams 24′. Thus, the single collimated, polychromatic optical output beam 26′ is a single collimated, multiplexed, polychromatic optical output beam 26′. The diffractive optic collimating/focusing lens 16 focuses the single collimated, multiplexed, polychromatic optical output beam 26′, and then transmits the resulting single multiplexed, polychromatic optical output beam 26 to the output fiber coupling device 20 where it becomes incident upon the single optical output fiber 22. The single multiplexed, polychromatic optical output beam 26 is then coupled into single optical output fiber 22 for transmission therethrough.

At this point it should again be noted that the input fiber coupling device 14 and the output fiber coupling device 20 are disposed offset from, but symmetrically about, the optical axis X—X of the multiplexing device 10 so as to insure that the single multiplexed, polychromatic optical output beam 26 is directed to the single optical output fiber 22 secured to the output fiber coupling device 20. However, in addition to this offset spacing of the input fiber coupling device 14 and the output fiber coupling device 20, the single multiplexed, polychromatic optical output beam 26 is also insured of being directed to the single optical output fiber 22 in a very efficient manner (i.e., with very low insertion losses and negligible channel crosstalk) by virtue of the enhanced imaging of both the input optical beams 24 and output optical beam 26 within the multiplexing device 10 through the use of the diffractive optic collimating/focusing lens 16. This enhanced imaging of both the input optical beams 24 and output optical beam 26 within the multiplexing device 10 is a direct result of the collimating/focusing lens 16 being a diffractive optic type lens rather than a refractive optic type lens, as described in more detail below.

There are two basic types of transmission optics: refractive optics and diffractive optics. Heretofore, most lenses have been refractive optic lenses, which have been used in applications such as, for example, eyeglasses, microscopes, and binoculars. A refractive optic lens is typically fabricated such that the lens material (e.g., glass, crystalline, or plastic) has a varying thickness and smooth, spherical curved surfaces. Incoming light is bent or refracted based upon the angle of incidence of the incoming light and the change in refractive index at each lens surface. To a lesser extent, differences in the thickness of the lens material also affect the degree to which incoming light is bent. To bend incoming light at a large angle, both a steep curvature and a large refractive index change at a lens surface are required. Typically, multiple refractive optic lenses are necessary to bend light to the degree required for collimating or focusing light. However, aberrations resulting from the use of spherical lenses often cause actual performance to be significantly less than desired for demanding optical designs, including WDM devices of the basic design described herein. To remedy this problem, lens-makers typically craft expensive and difficult-to-make nonspherical lenses.

A diffractive optic lens, on the other hand, works by breaking up an incoming wave of light into a large number of wavelets, which recombine to form a completely new wave or waves at an exit surface of the diffractive optic lens. The new wave(s) can move in a direction that is the same as or different from the direction of the incoming light wave depending upon the profile of the diffractive optic lens. A diffractive optic lens can also convert a single input light beam into multiple output light beams, focus an input light beam onto a point or into a pattern, homogenize an input light beam, or diffuse an input light beam into a controlled area.

A diffractive optic lens breaks up an incoming light wave by forcing it through a microscopic pattern that is formed on a surface of the lens material (e.g., glass, crystalline, or plastic). The microscopic pattern is typically formed on the surface of the lens material using a photolithography process. It should be noted that the microscopic pattern can also be applied, transferred, or replicated onto a lens or substrate surface using optical cement or some other optically transparent bonding technique. The microscopic pattern can take many forms but, for the purpose of collimating and focusing light beams in accordance with the present invention, the microscopic pattern may take the form of a concentric circular pattern of steps or peaks surrounding a center raised region, all being centered about an optical axis. One type of diffractive optic lens is a binary diffractive optic lens, which generally has block-like steps. Another type of diffractive optic lens is a Fresnel diffractive optic lens, which generally has curved peaks. Referring to FIG. 2a, there is shown an end and a cross-sectional view of a binary diffractive optic lens 116 having a concentric circular pattern of steps 118 surrounding a center raised region 120. In FIG. 2a, the microscopic pattern is shown etched into the lens material. Referring to FIG. 2b, there is shown an end and a cross-sectional view of a Fresnel diffractive optic lens 216 having a concentric circular pattern of peaks 218 surrounding a center raised region 220. In FIG. 2b, the microscopic pattern is shown applied to the lens material. The size and spacing of the stairs, peaks, and center raised region determine how the incoming light will be affected, as is commonly known in the art. In general, the size of the features is on the order of the wavelength of the light that is incident on the lens.

At this point it should be noted that the microscopic pattern need only be formed on one surface of a diffractive optic lens. That is, the microscopic pattern need only be formed on either the front or back surface of a diffractive optic lens in order for the lens to be functional. Also, the microscopic pattern that is formed on a diffractive optic lens is indeed microscopic such that the surface having the microscopic pattern is typically substantially planar. The surface not having the microscopic pattern is also typically substantially planar. The fact that both surfaces of a diffractive optic lens (i.e., the front patterned surface and the back unpatterned surface, or vice versa) are typically substantially planar is an important aspect of the present invention when forming an integrated device using one or more diffractive optic lenses, as described in more detail below.

A diffractive optic lens can typically achieve 90 percent or greater focusing or coupling efficiency, and while a conventional refractive optic lens commonly requires one or more lenses together to bend light, a diffractive optic lens can perform the same function with a thickness as small as a thousandth of a millimeter. Also, by choosing the appropriate steepness and spacing of the steps or the peaks, it is possible to avoid or eliminate problems such as spherical and other types of aberrations. Furthermore, diffractive optic lenses, when produced in large quantities, are often significantly cheaper and more uniform than refractive optic lenses for performing even relatively simple optical functions such as collimating and focusing. Additionally, once an original diffractive optic lens has been fabricated, it can be reproduced through embossing, plastic injection molding, or batch photolithographic processing, thereby reducing the cost of multiple diffractive optic lenses.

At this point it should be noted that the plurality of optical input fibers 12 could be replaced in the multiplexing device 10 by a corresponding plurality of laser diodes 28 secured within a coupling device 30, such as shown in FIG. 3a. The coupling device 30 performs a similar function to the input fiber coupling device 14, that being to precisely group the plurality of laser diodes 28 into a one-dimensional input array. The plurality of laser diodes 28 are used in place of the plurality of optical input fibers 12 to transmit the plurality of monochromatic optical input beams 24 to the multiplexing device 10. The array of laser diodes 28 may operate alone, or may be used with appropriate focusing lenses to provide the best coupling and the lowest amount of signal loss and channel crosstalk.

At this point it should be noted that the multiplexing device 10, as well as all of the multiplexing devices described herein, may be operated in a converse configuration as a demultiplexing device 40, such as shown in FIGS. 4a and 4 b. The demultiplexing device 40 is physically identical to the multiplexing device 10, and is therefore numerically identified as such. However, the demultiplexing device 40 is functionally opposite to the multiplexing device 10. That is, a single multiplexed, polychromatic optical input beam 42 is transmitted from the single optical fiber 22, and a plurality of monochromatic optical output beams 44 are transmitted to the plurality of optical fibers 12, wherein each one of the plurality of monochromatic optical output beams 44 is transmitted to a corresponding one of the plurality of optical fibers 12. The single multiplexed, polychromatic optical input beam 42 is simultaneously carrying a plurality of channels of data, each at a unique wavelength which is preferably, but not required to be, within the infrared (IR) region of the electromagnetic spectrum. The plurality of monochromatic optical output beams 44 are each carrying a single channel of data at a corresponding one of the unique wavelengths of the single multiplexed, polychromatic optical input beam 42. The single multiplexed, polychromatic optical input beam 42 is separated into the plurality of monochromatic optical output beams 44 through the combined operation of the diffractive optic collimating/focusing lens 16 and the reflective diffraction grating 18. Thus, the diffractive optic collimating/focusing lens 16 and the reflective diffraction grating 18 operate to perform a demultiplexing function.

At this point it should be noted that the plurality of optical fibers 12 could be replaced in the demultiplexing device 40 by a corresponding plurality of photodetectors 48 secured within a coupling device 50, such as shown in FIG. 3b. The coupling device 50 performs a similar function to the fiber coupling device 14, that being to precisely group the plurality of photodetectors 48 into a one-dimensional input array. The plurality of photodetectors 48 are used in place of the plurality of optical fibers 12 to receive the plurality of monochromatic optical output beams 44 from the demultiplexing device 40. The array of photodetectors 48 may operate alone, or may be used with appropriate focusing lenses to provide the best coupling and the lowest amount of signal loss and channel crosstalk.

Referring to FIGS. 5a and 5 b, there are shown a side view and a top view, respectively, of an alternate embodiment of a wavelength division multiplexing device 60 in accordance with the present invention. The multiplexing device 60 is physically identical to the multiplexing device 10, except for the addition of a first homogeneous index boot lens 62 between the fiber coupling devices 14, 20 and the diffractive optic collimating/focusing lens 16, and a second homogeneous index boot lens 64 between the diffractive optic collimating/focusing lens 16 and the reflective diffraction grating 18. The first homogeneous index boot lens 62 and the second homogeneous index boot lens 64 are preferably fabricated, for example, of fused silica (n=1.444), although numerous other optical glass materials may also be used.

The first homogeneous index boot lens 62 has a planar front surface 62 a for mating with the fiber coupling devices 14 and 20 and the associated secured optical fibers 12 and 22, respectively. The fiber coupling devices 14 and 20 and the secured optical fibers 12 and 22 may be either abutted against the planar front surface 62 a or affixed to the planar front surface 62 a using optical cement or some other optically transparent bonding technique, depending upon system mobility requirements and optical beam alignment and loss considerations.

The first homogeneous index boot lens 62 also has a planar back surface 62 b for mating with a planar front surface 16 a of the diffractive optic collimating/focusing lens 16. The planar back surface 62 b of the first homogeneous index boot lens 62 is typically joined or affixed to the planar front surface 16 a of the diffractive optic collimating/focusing lens 16 using optical cement or some other optically transparent bonding technique.

The second homogeneous index boot lens 64 has a planar front surface 64 a for mating with a planar back surface 16 b of the diffractive optic collimating/focusing lens 16. The planar front surface 64 a of the second homogeneous index boot lens 64 is typically joined or affixed to the planar back surface 16 b of the diffractive optic collimating/focusing lens 16 using optical cement or some other optically transparent bonding technique.

The second homogeneous index boot lens 64 also has a planar back surface 64 b that is angled similar to the reflective diffraction grating 18 at the Littrow diffraction angle, α_(i), relative to the optical axis X—X of the multiplexing device 60. As with the multiplexing device 10, the reflective diffraction grating 18 can be formed using a separate material, and this material can then be joined or affixed to the planar back surface 64 b of the second homogeneous index boot lens 64 using optical cement or some other optically transparent bonding technique. Alternatively, the reflective diffraction grating 18 can be formed directly on the planar back surface 64 b of the second homogeneous index boot lens 64, thereby avoiding the joining or affixing of the reflective diffraction grating 18 to the planar back surface 64 b of the second homogeneous index boot lens 64. In either case, the reflective diffraction grating 18 and the second homogeneous index boot lens 64 are integrated along with the diffractive optic collimating/focusing lens 16 and the first homogeneous index boot lens 62 to form a compact, rigid, and environmentally and thermally stable multiplexing device 60. The integrated nature of this multiplexing device 60 is particularly useful for maintaining component alignment, which provides long-term performance in contrast to some non-integrated air-spaced devices that characteristically degrade in alignment and therefore performance over time.

At this point it should be noted that, as previously described, the microscopic pattern can be formed on either the planar front surface 16 a or the planar back surface 16 b of the diffractive optic collimating/focusing lens 16 without substantially changing the planar characteristics of that surface. Thus, regardless of which surface possesses the microscopic pattern, the planar characteristics of both the planar front surface 16 a and the planar back surface 16 b of the diffractive optic collimating/focusing lens 16 allow for easy mating and integrated assembly with the planar back surface 62 b of the first homogeneous index boot lens 62 and the planar front surface 64 a of the second homogeneous index boot lens 64, respectively. These planar characteristics of the diffractive optic collimating/focusing lens 16 are particularly beneficial when viewed in comparison to a refractive optic lens, which typically has at least one curved surface.

The multiplexing device 60 is functionally identical to the multiplexing device 10, except for a slight decrease in optical beam transmission efficiency due to the addition of the first and second homogeneous index boot lenses 62 and 64, respectively. However, even with this slight decrease in optical beam transmission efficiency, the optical performance of the multiplexing device 60 is still exceptional due to the use of a diffractive optic type lens instead of a refractive optic type lens for the collimating/focusing lens 16. That is, as previously described, the use of a diffractive optic type lens for the collimating/focusing lens 16 can be used to eliminate aberrations caused by the spherical nature of a refractive optic type lens. And these aberrations are still eliminated despite the addition of the first and second homogeneous index boot lenses 62 and 64, respectively.

Referring to FIGS. 6a and 6 b, there are shown a side view and a top view, respectively, of an alternate embodiment of a wavelength division multiplexing device 70 in accordance with the present invention. The multiplexing device 70 is physically identical to the multiplexing device 60, except that the first homogeneous index boot lens 62 has been removed and the planar front surface 16′a of the diffractive optic collimating/focusing lens 16′ has been extended so as to allow the fiber coupling devices 14, 20 and the secured optical fibers 12 and 22, respectively, to be either abutted against the planar front surface 16′a or affixed to the planar front surface 16′a using optical cement or some other optically transparent bonding technique, depending upon system mobility requirements and optical beam alignment and loss considerations. In this case, the microscopic pattern is formed on the planar back surface 16′b of the diffractive optic collimating/focusing lens 16′ without substantially changing the planar characteristics of that surface. Similar to the multiplexing device 60, the integrated nature of the multiplexing device 70 is particularly useful for maintaining component alignment, which provides long-term performance in contrast to some non-integrated air-spaced devices that characteristically degrade in alignment and therefore performance over time. The multiplexing device 70 is functionally identical to the multiplexing device 60, except for a slight increase in optical beam transmission efficiency due to the removal of the first homogeneous index boot lens 62.

Referring to FIGS. 7a and 7 b, there are shown a side view and a top view, respectively, of an alternate embodiment of a wavelength division multiplexing device 80 in accordance with the present invention. The multiplexing device 80 is physically identical to the multiplexing device 60, except that the second homogeneous index boot lens 64 has been removed and the planar back surface 16″b of the diffractive optic collimating/focusing lens 16″ has been extended out to the reflective diffraction grating 18 and angled similar to the reflective diffraction grating 18 at the Littrow diffraction angle, α_(i), relative to the optical axis X—X of the multiplexing device 80. In this case, the microscopic pattern is formed on the planar front surface 16″a of the diffractive optic collimating/focusing lens 16″ without substantially changing the planar characteristics of that surface. As with the multiplexing device 10, the reflective diffraction grating 18 can be formed using a separate material, and this material can then be joined or affixed to the planar back surface 16″b of the diffractive optic collimating/focusing lens 16″ using optical cement or some other optically transparent bonding technique. Alternatively, the reflective diffraction grating 18 can be formed directly on the planar back surface 16″b of the diffractive optic collimating/focusing lens 16″, thereby avoiding the joining or affixing of the reflective diffraction grating 18 to the planar back surface 16″b of the diffractive optic collimating/focusing lens 16″. In either case, the reflective diffraction grating 18 and the diffractive optic collimating/focusing lens 16″ are integrated along with the first homogeneous index boot lens 62 to form a compact, rigid, and environmentally and thermally stable multiplexing device 80. Similar to the multiplexing device 60, the integrated nature of the multiplexing device 80 is particularly useful for maintaining component alignment, which provides long-term performance in contrast to some non-integrated air-spaced devices that characteristically degrade in alignment and therefore performance over time. The multiplexing device 80 is functionally identical to the multiplexing device 60, except for a slight increase in optical beam transmission efficiency due to the removal of the second homogeneous index boot lens 64.

At this point it should be noted that either the first homogeneous index boot lens 62 or the second homogeneous index boot lens 64 may be removed from the multiplexing device 60, the second homogeneous index boot lens 64 may be removed from the multiplexing device 70, and the first homogeneous index boot lens 62 may be removed from the multiplexing device 80 in order to create additional alternate embodiments (not shown) while still retaining the above-described benefits of using a diffractive optic type lens instead of a refractive optic type lens for the collimating/focusing lens 16.

Referring to FIG. 8, there is shown a side view of an alternate embodiment of a wavelength division multiplexing device 100 in accordance with the present invention. The multiplexing device 100 differs from the previously described embodiments by using a separate diffractive optic collimating lens 102, a separate diffractive optic focusing lens 106, and a reflective diffraction grating 104 that is configured to operate at reflecting angle that is different than the reflecting angle of the previously described embodiments. The diffractive optic collimating lens 102 collimates the plurality of monochromatic optical input beams 24, and then transmits the plurality of collimated, monochromatic optical input beams 24′ to the reflective diffraction grating 104. The reflective diffraction grating 104 removes the angular separation from the plurality of collimated, monochromatic optical input beams 24′ and reflects the single collimated, multiplexed, polychromatic optical output beam 26′ toward the diffractive optic focusing lens 106. The diffractive optic focusing lens 106 focuses the single collimated, multiplexed, polychromatic optical output beam 26′, and then transmits the resulting single multiplexed, polychromatic optical output beam 26 to the output fiber coupling device 20 where it becomes incident upon the single optical output fiber 22. The single multiplexed, polychromatic optical output beam 26 is then coupled into the single optical output fiber 22 for transmission therethrough.

In accordance with the practices described above, homogeneous index boot lenses can be added to the multiplexing device 100 and/or either one of the diffractive optic collimating lens 102 or the diffractive optic focusing lens 106 can be extended so as to allow the fiber coupling device 14 and the secured optical fibers 12 or the fiber coupling device 20 and the secured optical fibers 22, respectively, to be either abutted against the planar front surface of the diffractive optic collimating lens 102 or the diffractive optic focusing lens 106 or affixed to the planar front surface of the diffractive optic collimating lens 102 or the diffractive optic focusing lens 106 using optical cement or some other optically transparent bonding technique, depending upon system mobility requirements and optical beam alignment and loss considerations. The benefits and detriments associated with using these substitute/additional components are applicable to the multiplexing device 100 as would be the case with the embodiments described above. Of course, the most significant benefits come from the use of a diffractive optic type lens instead of a refractive optic type lens for the collimating lens 102 and the focusing lens 106. That is, regardless of embodiment, the use of diffractive optic type lenses in WDM devices yields increased device performance, as well as reduced device cost, complexity, and manufacturing risk. Simply said, the use of diffractive optic type lenses allows for the construction of a family of simple, low cost, yet very powerful WDM devices, particularly for use in DWDM (i.e., high channel number) applications.

At this point it should be noted that additional lenses can be added to the above described devices if such is required or desired to further increase the performance of the devices. For example, additional diffractive optic lenses or refractive optic lenses can be added to the above described devices if such is required to further increase the fiber coupling efficiency (FCE) of the devices. In contrast to a measure of insertion loss, the FCE of a WDM device expresses the efficiency of only the optical system of the WDM device for each data channel, without taking into account the efficiency of the diffraction grating. In these situations, a trade-off is typically made between a small increase in the FCE and the additional cost associated with adding additional lenses to a device.

The present invention is not to be limited in scope by the specific embodiments described herein. Indeed, various modifications of the present invention, in addition to those described herein, will be apparent to those of skill in the art from the foregoing description and accompanying drawings. Thus, such modifications are intended to fall within the scope of the appended claims. 

What is claimed is:
 1. An improved wavelength division multiplexing device having a diffraction grating for combining a plurality of monochromatic optical beams into a multiplexed, polychromatic optical beam, the improvement comprising: a diffractive optic collimating/focusing lens for collimating the plurality of monochromatic optical beams traveling along a first direction to the diffraction grating, and for focusing the multiplexed, polychromatic optical beam traveling along a second direction from the diffraction grating, the second direction being substantially opposite the first direction.
 2. The improved wavelength division multiplexing device as defined in claim 1, wherein the diffractive optic collimating/focusing lens operates in the infrared region of the electromagnetic spectrum.
 3. The improved wavelength division multiplexing device as defined in claim 1, wherein the diffractive optic collimating/focusing lens has substantially planar front and back surfaces.
 4. The improved wavelength division multiplexing device as defined in claim 3, wherein a microscopic pattern is formed on the substantially planar front surface.
 5. The improved wavelength division multiplexing device as defined in claim 3, wherein a microscopic pattern is formed on the substantially planar back surface.
 6. The improved wavelength division multiplexing device as defined in claim 1, wherein the diffractive optic collimating/focusing lens is formed of a material selected from the group consisting of glass, crystalline, and is plastic.
 7. The improved wavelength division multiplexing device as defined in claim 1, wherein the diffractive optic collimating/focusing lens is a binary diffractive optic lens.
 8. The improved wavelength division multiplexing device as defined in claim 1, wherein the diffractive optic collimating/focusing lens is a Fresnel diffractive optic lens.
 9. The improved wavelength division multiplexing device as defined in claim 1, wherein the diffraction grating is a reflective diffraction grating oriented at the Littrow diffraction angle with respect to the first and second directions.
 10. An improved wavelength division multiplexing device having a diffraction grating for combining a plurality of monochromatic optical beams into a multiplexed, polychromatic optical beam, the improvement comprising: a diffractive optic collimating lens for collimating the plurality of monochromatic optical beams traveling along a first direction to the diffraction grating; and a diffractive optic focusing lens for focusing the multiplexed, polychromatic optical beam traveling along a second direction from the diffraction grating, the second direction being different from the first direction.
 11. An improved wavelength division demultiplexing device having a diffraction grating for separating a multiplexed, polychromatic optical beam into a plurality of monochromatic optical beams, the improvement comprising: a diffractive optic collimating/focusing lens for collimating the multiplexed, polychromatic optical beam traveling along a first direction to the diffraction grating, and for focusing the plurality of monochromatic optical beams traveling along a second direction from the diffraction grating, the second direction being substantially opposite the first direction.
 12. The improved wavelength division demultiplexing device as defined in claim 11, wherein the diffractive optic collimating/focusing lens operates in the infrared region of the electromagnetic spectrum.
 13. The improved wavelength division demultiplexing device as defined in claim 11, wherein the diffractive optic collimating/focusing lens has substantially planar front and back surfaces.
 14. The improved wavelength division demultiplexing device as defined in claim 13, wherein a microscopic pattern is formed on the substantially planar front surface.
 15. The improved wavelength division demultiplexing device as defined in claim 13, wherein a microscopic pattern is formed on the substantially planar back surface.
 16. The improved wavelength division demultiplexing device as defined in claim 11, wherein the diffractive optic collimating/focusing lens is formed of a material selected from the group consisting of glass, crystalline, and plastic.
 17. The improved wavelength division demultiplexing device as defined in claim 11, wherein the diffractive optic collimating/focusing lens is a binary diffractive optic lens.
 18. The improved wavelength division demultiplexing device as defined in claim 11, wherein the diffractive optic collimating/focusing lens is a Fresnel diffractive optic lens.
 19. The improved wavelength division demultiplexing device as defined in claim 11, wherein the diffraction grating is a reflective diffraction grating oriented at the Littrow diffraction angle with respect to the first and second directions.
 20. An improved wavelength division demultiplexing device having a diffraction grating for separating a multiplexed, polychromatic optical beam into a plurality of monochromatic optical beams, the improvement comprising: a diffractive optic collimating lens for collimating the multiplexed, polychromatic optical beam traveling along a first direction to the diffraction grating; and a diffractive optic focusing lens for focusing the plurality of monochromatic optical beams traveling along a second direction from the diffraction grating, the second direction being different from the first direction.
 21. An integrated wavelength division multiplexing device comprising: a diffractive optic collimating/focusing lens for collimating a plurality of monochromatic optical beams traveling along a first direction, and for focusing a multiplexed, polychromatic optical beam traveling along a second direction, the second direction being substantially opposite the first direction; a homogeneous index boot lens affixed to the diffractive optic collimating/focusing lens for transmitting the plurality of monochromatic optical beams from the diffractive optic collimating/focusing lens along the first direction, and for transmitting the multiplexed, polychromatic optical beam to the diffractive optic collimating/focusing lens along the second direction, the homogeneous index boot lens having a planar interface surface; and a diffraction grating formed at the planar interface surface of the homogeneous index boot lens for combining the plurality of monochromatic optical beams into the multiplexed, polychromatic optical beam, and for reflecting the multiplexed, polychromatic optical beam back into the homogeneous index boot lens.
 22. The device as defined in claim 21, wherein the homogeneous index boot lens is incorporated into the diffractive optic collimating/focusing lens such that the diffractive optic collimating/focusing lens has the planar interface surface at which the diffraction grating is formed.
 23. The device as defined in claim 21, wherein the homogeneous index boot lens is a first homogeneous index boot lens, the device further comprising: a second homogeneous index boot lens affixed to the diffractive optic collimating/focusing lens for transmitting the plurality of monochromatic optical beams to the diffractive optic collimating/focusing lens along the first direction, and for transmitting the multiplexed, polychromatic optical beam from the diffractive optic collimating/focusing lens along the second direction.
 24. The device as defined in claim 23, wherein the second homogeneous index boot lens has a planar interface surface for accepting the plurality of monochromatic optical beams from at least one optical source, and for outputting the multiplexed, polychromatic optical beam to at least one optical receiver.
 25. The device as defined in claim 21, wherein the diffractive optic collimating/focusing lens has a planar interface surface for accepting the plurality of monochromatic optical beams from at least one optical source, and for outputting the multiplexed, polychromatic optical beam to at least one optical receiver.
 26. The device as defined in claim 21, wherein the diffraction grating is a reflective diffraction grating oriented at the Littrow diffraction angle with respect to the first and second directions.
 27. An integrated wavelength division demultiplexing device comprising: a diffractive optic collimating/focusing lens for collimating a multiplexed, polychromatic optical beam is traveling along a first direction, and for focusing a plurality of monochromatic optical beams traveling along a second direction, the second direction being substantially opposite the first direction; a homogeneous index boot lens affixed to the diffractive optic collimating/focusing lens for transmitting the multiplexed, polychromatic optical beam from the diffractive optic collimating/focusing lens along the first direction, and for transmitting the plurality of monochromatic optical beams to the diffractive optic collimating/focusing lens along the second direction, the homogeneous index boot lens having a planar interface surface; and a diffraction grating formed at the planar interface surface of the homogeneous index boot lens for separating the multiplexed, polychromatic optical beam into the plurality of monochromatic optical beams, and for reflecting the plurality of monochromatic optical beams back into the homogeneous index boot lens.
 28. The device as defined in claim 27, wherein the homogeneous index boot lens is incorporated into the diffractive optic collimating/focusing lens such that the diffractive optic collimating/focusing lens has the planar interface surface at which the diffraction grating is formed.
 29. The device as defined in claim 27, wherein the homogeneous index boot lens is a first homogeneous index boot lens, the device further comprising: a second homogeneous index boot lens affixed to the diffractive optic collimating/focusing lens for transmitting the multiplexed, polychromatic optical beam to the diffractive optic collimating/focusing lens along the first direction, and for transmitting the plurality-of monochromatic optical beams from the diffractive optic collimating/focusing lens along the second direction.
 30. The device as defined in claim 29, wherein the second homogeneous index boot lens has a planar interface surface for accepting the multiplexed, polychromatic optical beam from an optical source, and for outputting the plurality of monochromatic optical beams to at least one optical receiver.
 31. The device as defined in claim 27, wherein the diffractive optic collimating/focusing lens has a planar interface surface for accepting the multiplexed, polychromatic optical beam from an optical source, and for outputting the plurality of monochromatic optical beams to at least one optical receiver.
 32. The device as defined in claim 27, wherein the diffraction grating is a reflective diffraction grating oriented at the Littrow diffraction angle with respect to the first and second directions.
 33. A wavelength division multiplexing device comprising: a diffractive optic collimating lens for collimating a plurality of monochromatic optical beams; a diffraction grating for combining the plurality of collimated, monochromatic optical beams into a multiplexed, polychromatic optical beam, and for reflecting the multiplexed, polychromatic optical beam; and a diffractive optic focusing lens for focusing the reflected, multiplexed, polychromatic optical beam.
 34. The device as defined in claim 33, further comprising: at least one reflecting element for reflecting the plurality of collimated, monochromatic optical beams toward the diffraction grating.
 35. The device as defined in claim 33, further comprising: at least one reflecting element for reflecting the reflected, multiplexed, polychromatic optical beam toward the diffractive optic focusing lens.
 36. A wavelength division demultiplexing device comprising: a diffractive optic collimating lens for collimating a multiplexed, polychromatic optical beam; a diffraction grating for separating the collimated, multiplexed, polychromatic optical beam into a plurality of monochromatic optical beams, and for reflecting the plurality of monochromatic optical beams; and a diffractive optic focusing lens for focusing the plurality of reflected, monochromatic optical beams.
 37. The device as defined in claim 36, further comprising: at least one reflecting element for reflecting the collimated, multiplexed, polychromatic optical beam toward the diffraction grating.
 38. The device as defined in claim 36, further comprising: at least one reflecting element for reflecting the plurality of reflected, monochromatic optical beams toward the diffractive optic focusing lens. 